Henry D Herce1, Angel E Garcia, M Cristina Cardoso. 1. Department of Physics, Applied Physics and Astronomy and Center for Biotechnology and Interdisciplinary Studies, Rensselaer Polytechnic Institute , Troy, New York 12180, United States.
Abstract
Guanidinium-rich molecules, such as cell-penetrating peptides, efficiently enter living cells in a non-endocytic energy-independent manner and transport a wide range of cargos, including drugs and biomarkers. The mechanism by which these highly cationic molecules efficiently cross the hydrophobic barrier imposed by the plasma membrane remains a fundamental open question. Here, a combination of computational results and in vitro and live-cell experimental evidence reveals an efficient energy-independent translocation mechanism for arginine-rich molecules. This mechanism unveils the essential role of guanidinium groups and two universal cell components: fatty acids and the cell membrane pH gradient. Deprotonated fatty acids in contact with the cell exterior interact with guanidinium groups, leading to a transient membrane channel that facilitates the transport of arginine-rich peptides toward the cell interior. On the cytosolic side, the fatty acids become protonated, releasing the peptides and resealing the channel. This fundamental mechanism appears to be universal across cells from different species and kingdoms.
Guanidinium-rich molecules, such as cell-penetrating peptides, efficiently enter living cells in a non-endocytic energy-independent manner and transport a wide range of cargos, including drugs and biomarkers. The mechanism by which these highly cationic molecules efficiently cross the hydrophobic barrier imposed by the plasma membrane remains a fundamental open question. Here, a combination of computational results and in vitro and live-cell experimental evidence reveals an efficient energy-independent translocation mechanism for arginine-rich molecules. This mechanism unveils the essential role of guanidinium groups and two universal cell components: fatty acids and the cell membrane pH gradient. Deprotonated fatty acids in contact with the cell exterior interact with guanidinium groups, leading to a transient membrane channel that facilitates the transport of arginine-rich peptides toward the cell interior. On the cytosolic side, the fatty acids become protonated, releasing the peptides and resealing the channel. This fundamental mechanism appears to be universal across cells from different species and kingdoms.
Cell-penetrating
peptides are short, usually arginine-rich amino
acid sequences that are capable of transporting a wide range of biomolecules
into virtually any living cell type.[1−8] There is abundant evidence that these peptides are able to directly
translocate across the plasma membrane in an energy-independent and
non-endocytotic manner, gaining free access to the cytosol and nucleus.[9−13] This challenges the fundamental concept that charged molecules cannot
spontaneously diffuse across the cell membrane. The mechanism behind
this puzzling effect follows three essential steps: (a) peptide binding
to plasma membrane components; (b) spontaneous peptide absorption
across the hydrophobic barrier imposed by the plasma membrane; and
(c) breakage of the strong ionic binding between the peptide and the
membrane when the peptide reaches the cytosol.Arginine-rich
peptides (RRPs) have strong affinities for multiple
negatively charged plasma membrane groups. This affinity is so strong
that removal of membrane-bound peptides requires enzymatic degradation
of the peptides and the addition of strong counterions such as heparin
to the wash solution.[14] However, it remains
unclear whether any of these multiple cell membrane components could
efficiently mediate the absorption of the RRPs into the hydrophobic
core of the plasma membrane. It has been suggested that some membrane
components could form stable complexes with RRPs, mediating their
absorption into the core of the plasma membrane by forming either
inverted micelles[15−17] or transient channels.[18−27] In both models, the peptides would reach the intracellular side
of the cell membrane strongly bound to the cell membrane. Therefore,
even if any of these mechanisms is right, there should be in place
a common cellular mechanism to release these peptides from the cell
membrane after they reach the cytosol.Herein is described a
complete cellular uptake mechanism for RRPs
based on the ubiquitous interplay between two universal cell components:
fatty acids and the plasma membrane pH gradient. We propose that at
high pH fatty acids bind extracellular RRPs, mediate their membrane
transport, and release them into the lower-pH environment of the cytosol.
In vitro experiments presented here show all of the major steps of
this mechanism. Computational results show that deprotonated fatty
acids reduce the free energy of insertion of RRPs into model phospholipid
bilayers and that this insertion leads to the formation of a channel
across the lipid bilayer. Accordingly, live-cell experiments show
that both the extracellular pH and the cell membrane fatty acid content
modulate the cell transduction of RRPs into living cells. Furthermore,
this mechanism describes the puzzling cell uptake differences observed
between polyarginine and polylysine peptides. Finally, peptide uptake
observations in multiple cell lines and the universality of the elements
involved in this model (fatty acids and the cell pH gradient) suggest
that this mechanism is universal across cells from different species
and kingdoms.
Results and Discussion
Protonation State of Fatty Acids Modulates
RRP Binding
The central hypothesis of this work is that fatty
acids can simultaneously mediate RRP membrane binding, membrane insertion,
and cytosolic release. We postulate that this process is triggered
by the pH gradient across the plasma membrane.A simple in vitro
model system to test this hypothesis is to study the distribution
of RRPs between an aqueous buffer and octanol. Figure 1a shows a photograph displaying an aqueous buffer at different
pHs in contact with an octanol phase containing 1% oleic acid. At
pH less than 6.75, the TATpeptide (an RRP derived from the HIV-1
TAT protein) partitions mainly into the aqueous phase, while at any
pH larger than 6.75, the TATpeptide is absorbed into the octanol
phase. The plot shows the fluorescence emission intensity of the peptide
labeled with TAMRA in each phase and at each pH value of the buffer.
This indicates that fatty acids change from being neutral (protonated)
at low pH to negatively charged (deprotonated) at high pH. Remarkably,
the peptide absorption into the hydrophobic phase can be modulated
within a physiological range very close to the extra- and intracellular
pH in mammalian cells.
Figure 1
Within a physiological
pH range, arginine-rich peptides can partition
into an aqueous buffer at low pH and a hydrophobic environment at
high pH. (a) Photograph showing that at pH less than 6.75 the TAT
peptide (10 μM), labeled with TAMRA, partitions mainly into
the aqueous phase, while at any pH higher than 6.75 the TAT peptide
partitions mainly into the phase composed of octanol and 1% oleic
acid. The plot shows the fluorescence emission of the peptide in each
phase for each pH. While arginine and lysine amino acids do not change
their protonation state within this range, fatty acids change from
being neutral (protonated) at low pH to negatively charged (deprotonated)
at high pH. (b) Snapshots after 300 ns molecular dynamics simulations
of systems composed of 16 000 octanol molecules (represented
with a white transparent surface), 64 protonated (left) or deprotonated
(right) oleic acid molecules (the carbon chains of oleic acids are
colored in white, while oxygens of protonated oleic acid are colored
in gray and oxygens of deprotonated oleic acid are colored in green),
four peptides (in red), 24 000 water molecules (blue surface;
water molecules within 3 Å of any atom of the peptide or octanol
or fatty acids are explicitly shown in blue), and chloride (left)
or potassium (right) ions (in blue) to neutralize the system. When
the fatty acids are protonated, the TAT peptides are excluded from
the octanol phase, while when the fatty acids are deprotonated, the
peptides partition in the octanol phase surrounded by fatty acids
and water in a structure that resembles an inverted micelle.
Figure S1 in the Supporting Information shows as a control this partition for
the TAMRA dye alone, which
partially partitions into the octanol phase at pH lower than 6, while
for any higher pH the dye partitions only into the aqueous phase.
This is the opposite behavior as when the dye is coupled to the TATpeptide (Figure 1a), indicating that the peptides
drive the partition of the dyes into the aqueous phase at low pH and
into the hydrophobic phase at high pH.Within a physiological
pH range, arginine-rich peptides can partition
into an aqueous buffer at low pH and a hydrophobic environment at
high pH. (a) Photograph showing that at pH less than 6.75 the TATpeptide (10 μM), labeled with TAMRA, partitions mainly into
the aqueous phase, while at any pH higher than 6.75 the TATpeptide
partitions mainly into the phase composed of octanol and 1% oleic
acid. The plot shows the fluorescence emission of the peptide in each
phase for each pH. While arginine and lysine amino acids do not change
their protonation state within this range, fatty acids change from
being neutral (protonated) at low pH to negatively charged (deprotonated)
at high pH. (b) Snapshots after 300 ns molecular dynamics simulations
of systems composed of 16 000 octanol molecules (represented
with a white transparent surface), 64 protonated (left) or deprotonated
(right) oleic acid molecules (the carbon chains of oleic acids are
colored in white, while oxygens of protonated oleic acid are colored
in gray and oxygens of deprotonatedoleic acid are colored in green),
four peptides (in red), 24 000 water molecules (blue surface;
water molecules within 3 Å of any atom of the peptide or octanol
or fatty acids are explicitly shown in blue), and chloride (left)
or potassium (right) ions (in blue) to neutralize the system. When
the fatty acids are protonated, the TAT peptides are excluded from
the octanol phase, while when the fatty acids are deprotonated, the
peptides partition in the octanol phase surrounded by fatty acids
and water in a structure that resembles an inverted micelle.To obtain structural information
on the peptides absorbed into
the hydrophobic phase, we performed molecular dynamics simulations.
Figure 1b shows a system composed of octanol,
protonated (left) or deprotonated (right) oleic acid molecules, peptides,
water, and chloride or potassium ions to balance the charges. We can
see that when the fatty acids are protonated, the TAT peptides are
excluded from the octanol phase, while when the fatty acids are deprotonated,
the peptides partition into the octanol phase, forming a hydrophobic
complex surrounded by fatty acids with a hydrophilic interior composed
of water, ions, and the peptide. Therefore, peptides can be absorbed
into octanol by forming structures with fatty acids that resemble
inverted micelles with the polar groups in the interior of the structure.We next explored whether other groups and hydrophobic environments
would be able to modulate the absorption of arginine-rich peptides
within a physiological pH range.
Fatty
Acids Ubiquitously Modulate the Absorption
of RRPs into a Hydrophobic Environment within a Physiological pH Range
In the absence of oleic acid, TAT does not enter the hydrophobic
phase, as shown in Figure 2a. This indicates
that the pH change only modulates the protonation of fatty acids.
The pKa of simple carboxyl acids is around
4.5, such as formic acid (pKa = 3.77)
or acetic acid (pKa = 4.76), while the
pKa of fatty acids in pure monolayers
is around 10. The pKa, or apparent pKa, of fatty acids depends on several factors
such as the degree, type, and position of unsaturation and the local
environment,[28] and it has recently been
shown that in cells this value could be shifted toward a physiological
pH range.[29] On the other hand, the protonation
state of guanidinium groups is very stable even in hydrophobic environments.[30]
Figure 2
Fatty acids ubiquitously modulate the partition of arginine-rich
peptides within a physiological pH range. In the left column are shown
snapshots of microcentrifuge tubes containing the different hydrophobic
phases in contact with the aqueous buffers at different pHs. The right
column shows the structures of the relevant components. The TAT peptide
was labeled with TAMRA and excited with UV light (280 nm) to facilitate
the visualization of the peptide distribution. (a) In the absence
of carboxylic groups coupled to hydrophobic moieties, such as fatty
acids, the TAT peptide does not partition into octanol. (b) In the
presence of hydrophobic compounds containing phosphate and sulfur
groups (100 μM in octanol) the TAT peptide (10 μM) partitions
into the hydrophobic phase at every pH. These groups could help attract
the peptides toward the plasma membrane. However, these groups fail
to provide a mechanism for cytosolic release of membrane-bound peptides.
On the other hand, other hydrophobic molecules containing carboxyl
groups, such as lithocholic acid, display behavior similar to that
of oleic acid, although in this case the deprotonation is shifted
toward higher pH. (c) Partition of the TAT peptide into three distinct
types of natural vegetable oils: sunflower oil, castor oil, and olive
oil. Vegetable oils are rich in fatty acids. However, most of these
fatty acids are not free but instead form triglycerides, which lack
free carboxyl groups essential for the binding of RRPs.
Fatty acids ubiquitously modulate the partition of arginine-rich
peptides within a physiological pH range. In the left column are shown
snapshots of microcentrifuge tubes containing the different hydrophobic
phases in contact with the aqueous buffers at different pHs. The right
column shows the structures of the relevant components. The TATpeptide
was labeled with TAMRA and excited with UV light (280 nm) to facilitate
the visualization of the peptide distribution. (a) In the absence
of carboxylic groups coupled to hydrophobic moieties, such as fatty
acids, the TATpeptide does not partition into octanol. (b) In the
presence of hydrophobic compounds containing phosphate and sulfur
groups (100 μM in octanol) the TATpeptide (10 μM) partitions
into the hydrophobic phase at every pH. These groups could help attract
the peptides toward the plasma membrane. However, these groups fail
to provide a mechanism for cytosolic release of membrane-bound peptides.
On the other hand, other hydrophobic molecules containing carboxyl
groups, such as lithocholic acid, display behavior similar to that
of oleic acid, although in this case the deprotonation is shifted
toward higher pH. (c) Partition of the TATpeptide into three distinct
types of naturalvegetable oils: sunflower oil, castor oil, and olive
oil. Vegetable oils are rich in fatty acids. However, most of these
fatty acids are not free but instead form triglycerides, which lack
free carboxyl groups essential for the binding of RRPs.It has been speculated that membrane phosphate
and sulfur groups
might be critical for the cellular uptake of RRPs, but it can be seen
in Figure 2b that although these groups bind
to RRPs, they remain bound at every pH. These groups could help attract
the peptides toward the plasma membrane. However, they fail to provide
a mechanism for cytosolic release of membrane-bound peptides. Furthermore,
at the plasma membrane these groups are usually part of more complex
molecules such as plasma membrane phospholipids that are more rigid
and less likely to flip across the bilayer than simple fatty acids,
thus providing stability to the plasma membrane. At high concentrations,
these peptides can also penetrate and change the structure of phospholipid
membranes,[27] and their toxicity at high
concentrations might be a consequence of permanently destabilizing
the phospholipid bilayer. All of these factors make less favorable
the membrane absorption, translocation, and release of RRPs by complexation
with plasma membrane components containing phosphate or sulfur groups.
Figure 2b also shows that carboxyl groups present
in other types of amphiphilic molecules, such as lithocholic acid,
display behavior similar to that of oleic acid, although the deprotonation
in this case is shifted to a higher pH, suggesting that other molecules
containing a hydrophobic moiety coupled to carboxyl groups could analogously
modulate the absorption of arginine-rich molecules. This could help
explain recent works that have highlighted the specific role of pyrenebutyrate,
originally suggested by Sakai and Matile,[15] as an enhancer of the cellular uptake of RRPs.[31,32] This particular enhancer is composed of a carboxyl group (from the
butyric acid part of the molecule) followed by a hydrophobic structure
(mainly from the aromatic pyrene part).To explore these effects
in richer hydrophobic environments, we
also studied the partition of RRPs into three distinct types of naturalvegetable oils: sunflower oil, castor oil, and olive oil. Vegetable
oils are rich in fatty acids. However, most of these fatty acids are
not free but instead form triglycerides, which lack free carboxyl
groups essential for the binding of RRPs. We can see in Figure 2c that sunflower oil displays a behavior consistent
with a composition of only triglycerides, displaying no absorption
of the TATpeptide in the hydrophobic phase. Castor oil behaves as
also having free fatty acids, showing an absorption behavior similar
to that of oleic acid (Figure 1a). Olive oil
displays absorption of the TATpeptide at the interface at every pH,
revealing the presence of phospholipids.[33] This absorption remains constant until pH 6, followed by a clear
increase in absorption at higher pHs produced by the additional presence
of free fatty acids.We next adapted the previous in vitro setup
to test whether this
mechanism would allow the spontaneous transfer of RRPs from a high-
to a low-pH buffer across a hydrophobic barrier.
Fatty Acids Can Transport RRPs across a Hydrophobic
Barrier
The proton gradient across the cell membrane can
regulate fatty acid protonation and drive the cellular uptake of RRPs.
Therefore, we asked whether this effect could be captured in an analogous
in vitro assay. This assay should display the transport of cell-penetrating
peptides from a high-pH buffer to a low-pH buffer across a hydrophobic
barrier. Figure 3 shows that RRPs indeed diffuse
across the octanol hydrophobic barrier in the presence of fatty acids
from a high-pH to a low-pH buffer. Figure 3a shows a cartoon illustration of the in vitro setup and its cellular
analogue. The in vitro setup consists of two compartments at pH 7.5
and 4 connected by a layer of octanol with 1% oleic acid. Cells actively
control the pH gradient across the plasma membrane, while in this
experimental set up the pH is not actively maintained in each chamber.
This could potentially lead to a fast pH equilibration between the
two chambers as a consequence of the fatty-acid-mediated transfer
of protons. Therefore, we chose a lower pH for the trans compartment
than in the cytosol to ensure that the pH gradient between the two
compartments would be maintained throughout the experiment. The TAT
peptides were added to the pH 7.5 buffer. Figure 3b displays photographs of the setup at 2 h intervals and a
plot of the relative fluorescence intensity in each buffer at each
time point. After 2 h the peptides get absorbed initially into the
hydrophobic phase and then at a lower rate diffuse into the low-pH
chamber. After 6 h, the peptides are mostly distributed between the
octanol phase and the low-pH buffer. Therefore, fatty acids can mediate
the transport of RRPs across a hydrophobic environment from a high-
to a low-pH buffer, resembling the cellular uptake of RRPs. Furthermore,
the low-pH buffer can be considered a trap for the peptides, as the
peptides diffuse in one direction. The diffusion of the peptides across
the hydrophobic environment is primarily determined not by the peptide
concentration but instead by the proton concentration. This correlates
with the observation that RRPs diffuse toward the interior of cells
and that after the extracellular peptides are washed away the internalized
peptides remain trapped in the cells.
Figure 3
Arginine-rich cell-penetrating peptides
can diffuse across a hydrophobic
environment from a high- to a low-pH buffer in the presence of fatty
acids. (a) Cartoon description of the cellular analogue of the in
vitro setup, in which arginine-rich peptides are added to the extracellular
medium at higher pH and diffuse across the membrane barrier toward
the interior of cells at lower pH. The in vitro setup consists of
two compartments at pH 7.5 and 4 connected by a layer of octanol and
1% oleic acid. The peptides were added to the high-pH compartment
(pH 7.5), and they initially diffused into the hydrophobic phase and
then at a lower rate into the low-pH buffer (pH 4). (b) Photographs
of the setup and a plot of the peptide distribution (fluorescence
emission) at different times. After 6 h, the peptides were mostly
distributed between the octanol phase and the low-pH chamber.
Arginine-rich cell-penetrating peptides
can diffuse across a hydrophobic
environment from a high- to a low-pH buffer in the presence of fatty
acids. (a) Cartoon description of the cellular analogue of the in
vitro setup, in which arginine-rich peptides are added to the extracellular
medium at higher pH and diffuse across the membrane barrier toward
the interior of cells at lower pH. The in vitro setup consists of
two compartments at pH 7.5 and 4 connected by a layer of octanol and
1% oleic acid. The peptides were added to the high-pH compartment
(pH 7.5), and they initially diffused into the hydrophobic phase and
then at a lower rate into the low-pH buffer (pH 4). (b) Photographs
of the setup and a plot of the peptide distribution (fluorescence
emission) at different times. After 6 h, the peptides were mostly
distributed between the octanol phase and the low-pH chamber.We next asked how the protonation
of fatty acids affects the absorption
of RRPs in phospholipid bilayers.
Fatty
Acids Lower the Plasma Membrane Energetic
Barrier for RRPs
To understand how fatty acids affect the
peptide–membrane interaction in more detail, we computed the
free energy profiles for the insertion of a TATpeptide into model
phospholipid bilayers composed of a mixture of 1,2-dioleoyl-sn-glycero-3-phosphocholine (DOPC) and oleic acid. Umbrella
sampling was used to enhance the sampling along the free energy barrier
imposed by the lipid bilayer. Essentially, an external harmonic potential
was introduced, restraining the peptide at multiple positions across
the bilayer. The contribution of this bias to the free energy was
consistently removed using the WHAM method to obtain the free energy
required to insert the peptide into the bilayer.[34−36] Figure 4 shows the structures and free energy profiles of
three systems composed of a TATpeptide, water molecules, and a lipid
bilayer made of DOPC and oleic acid molecules. Figure 4a presents snapshots of the atomic conformations of the three
systems studied, with the peptide at the center of the bilayer. These
structures show that in the presence of deprotonated fatty acids the
peptide’s charged residues are screened by deprotonated fatty
acids that easily insert into the center bilayer. On the other hand,
in the absence of deprotonated fatty acids the arginine and lysine
residues cannot be easily screened at the center of the bilayer, leading
the peptide to acquire an extended conformation to reach the phosphate
groups of the more rigid phospholipids on the surface. Movies S1–S3
in the Supporting Information show structural
changes as the TATpeptide is inserted into the bilayer and the relative
free energy along this path for each case. These free energies are
plotted in Figure 4b, where it can be seen
that the addition of protonated fatty acids to the bilayer reduces
by half the reported[36] free energy of insertion
of the TATpeptide into pure DOPC bilayers. It can be seen that when
all of the fatty acids are deprotonated, the free energy barrier is
further reduced to 25 kJ/mol. This reduction is a consequence of efficient
screening of the arginine and lysine residues by deprotonated fatty
acids. This energetic barrier could be further reduced by the cell
transmembrane potential,[16,37,38] which is not necessary for the transport across octanol.
Figure 4
Structural
analysis and free energy computations for insertion
of the TAT peptide into phospholipid bilayers containing protonated
and deprotonated fatty acids using molecular dynamics simulations.
(a) Molecular conformations of the systems with the peptide constrained
at the center of the bilayer. The systems are composed of a TAT peptide,
8700 water molecules, 68 DOPC molecules, and 48 oleic acid molecules
(all protonated in red, half deprotonated in yellow, and all deprotonated
in green). The systems are neutralized with the addition of potassium
or chloride ions. Water is represented by a blue surface, with water
molecules less than 3 Å from any atom of the peptide or lipid
bilayer explicitly drawn in blue. DOPC and oleic acid molecules are
shown with a white surface. Phosphate atoms are shown in yellow, protonated
and deprotonated fatty acid carboxyl groups are shown in gray and
green, respectively, and the TAT peptide is shown in red. (b) Free
energy profiles as functions of the distance of the center of mass
of the TAT peptide from the center of mass of the lipid bilayer. The
total computed time for each free energy calculation profile was expanded
to 10 μs. (c) To see whether an inverted-micelle-like structure
would be stable at the center of the bilayer, we increased the bilayer
size by a factor of 4 and inserted a single TAT peptide surrounded
by water and oleic acid molecules that was previously equilibrated
within a mixture of octanol and deprotonated fatty acids (Figure 1b). The final system was composed of 272 DOPC molecules,
200 oleic acid molecules, potassium counterions, 34 800 water
molecules, and a TAT peptide. The peptide–fatty acid complex
obtained from the simulation shown in Figure 1b was placed in the middle of the bilayer. The layers of the bilayer
were separated, leaving significant space between the complex hydrophobic
core and the surface of the bilayer, and from this conformation the
systems relaxed to equilibrium for 150 ns at constant pressure. In
the two cases tested, the initial structure resembling a reverse micelle
transformed into a water-filled channel.
Structural
analysis and free energy computations for insertion
of the TATpeptide into phospholipid bilayers containing protonated
and deprotonated fatty acids using molecular dynamics simulations.
(a) Molecular conformations of the systems with the peptide constrained
at the center of the bilayer. The systems are composed of a TATpeptide,
8700 water molecules, 68 DOPC molecules, and 48 oleic acid molecules
(all protonated in red, half deprotonated in yellow, and all deprotonated
in green). The systems are neutralized with the addition of potassium
or chloride ions. Water is represented by a blue surface, with water
molecules less than 3 Å from any atom of the peptide or lipid
bilayer explicitly drawn in blue. DOPC and oleic acid molecules are
shown with a white surface. Phosphate atoms are shown in yellow, protonated
and deprotonatedfatty acid carboxyl groups are shown in gray and
green, respectively, and the TATpeptide is shown in red. (b) Free
energy profiles as functions of the distance of the center of mass
of the TATpeptide from the center of mass of the lipid bilayer. The
total computed time for each free energy calculation profile was expanded
to 10 μs. (c) To see whether an inverted-micelle-like structure
would be stable at the center of the bilayer, we increased the bilayer
size by a factor of 4 and inserted a single TATpeptide surrounded
by water and oleic acid molecules that was previously equilibrated
within a mixture of octanol and deprotonated fatty acids (Figure 1b). The final system was composed of 272 DOPC molecules,
200 oleic acid molecules, potassium counterions, 34 800 water
molecules, and a TATpeptide. The peptide–fatty acid complex
obtained from the simulation shown in Figure 1b was placed in the middle of the bilayer. The layers of the bilayer
were separated, leaving significant space between the complex hydrophobic
core and the surface of the bilayer, and from this conformation the
systems relaxed to equilibrium for 150 ns at constant pressure. In
the two cases tested, the initial structure resembling a reverse micelle
transformed into a water-filled channel.It has been proposed that a possible mechanism of insertion
of
RRPs into the core of the bilayer might involve the formation of reverse
micelles[39,40] with RRPs surrounded by ambiphilic counterions,
resembling the structure shown in Figure 1b.
However, we can see that in three independent simulations (Figure 4a), when a peptide is inserted in the center of
the bilayer, the lipid bilayer forms a water-channel structure.[18−20] To be sure that the system was not biased toward channel formation
by the computed system size or the initial structure, we performed
a new computation in which the system was enlarged and the initial
structure was biased toward the formation of an inverted-micelle-like
structure in the center of the bilayer. In Figure 4c, we increased the bilayer size by a factor of 4 and inserted
a single TATpeptide surrounded by water and deprotonatedoleic acid
using an initial structure from the simulations in Figure 1b resembling an inverted micelle. The peptide–fatty
acid complex obtained from the simulation shown in Figure 1b was placed in the middle of the bilayer. The layers
of the bilayer were separated, leaving significant space to fit the
inverted-micelle-like structure, and from this conformation the systems
relaxed at constant pressure to their final volume. In every case,
the systems relaxed spontaneously to form a channel. This further
supports that the insertion of RRPs into lipid bilayers leads to the
formation of channels.[18−20]Interestingly, it can also be observed that
protonated fatty acids
rapidly flip from one side of the bilayer to the other, while deprotonatedfatty acids do not flip within this time scale. If the extracellular
pH is much higher than the intracellular pH, any intracellular fatty
acid that becomes protonated in the cytosol would rapidly flip, get
deprotonated, and remain captured in the extracellular layer of the
cell membrane. This implies that increasing the extracellular pH would
greatly increase the number of deprotonated fatty acids in contact
with the external side of the plasma membrane, leading to an enhancement
of the cellular uptake of RRPs.Cells actively control the intracellular
pH, keeping it near neutral
pH, but the extracellular pH can be chemically controlled. Therefore,
we next asked whether altering the extracellular pH would modulate
the uptake of RRPs into living cells consistently with the previous
in vitro and molecular dynamics observations.
Extracellular
Proton Density Modulates the
Cellular Uptake of RRPs
Fatty acids are an integral part
of all known cells. If this mechanism is also present in cells, then
raising (lowering) the extracellular pH should enhance (reduce) the
transduction of these peptides. Therefore, as shown in Figure 5 and movies S4–S9 in the Supporting Information, we compared the uptake of the TATpeptide when the extracellular pH was chemically controlled at different
values. In most mammalian cells, the extracellular pH is close to
7.4. Therefore, we studied the peptide uptake in HeLa cells with the
extracellular pH kept at 6, 7.5, and 9 using a HEPES buffer. Figure 5 shows time-lapse confocal microscopy snapshots
of the uptake of the TATpeptide in living cells. While at this TATpeptide concentration (2 mM) there was no uptake at pH 6 and 7.5,
most of the cells kept at pH 9 displayed significant uptake within
this time interval (30 min). We also measured the change in the average
fluorescence intensity of the entire image minus the background fluorescence
(Figure 5), and we can see that at pH 6 and
7.5 this value remains negative, indicating that the concentration
of membrane-bound and/or intracellular peptide is less than that in
the extracellular medium, while at pH 9 the curve is positive, indicating
clear cellular uptake.
Figure 5
Increasing the extracellular pH consistently increases
the transduction
efficiency of arginine-rich peptides. Time-lapse fluorescence images
show the TAT (2 μM) uptake in living cells at pH 6, 7.5, and
9. The lower plot shows the averages (over three independent repetitions)
of the overall fluorescence intensity minus the background intensity
and the standard errors of the mean as functions of time. After 30
min the fluorescence increased several-fold at pH 9 relative to pH
6 and 7.5. The images were acquired using an objective with 20×
magnification. In this case, the membrane-bound peptide cannot be
separated from the internalized peptide. To measure more strictly
the free intracellular distributed peptide and compare it with these
results, we simultaneously imaged the cells in the dotted regions
using an objective with 60× magnification (Figure S2 in the Supporting Information). We measured the fluorescence
intensity at the nucleolus relative to the background fluorescence
over time and found that the two measurements gave analogous results.
Scale bars = 75 μm.
Increasing the extracellular pH consistently increases
the transduction
efficiency of arginine-rich peptides. Time-lapse fluorescence images
show the TAT (2 μM) uptake in living cells at pH 6, 7.5, and
9. The lower plot shows the averages (over three independent repetitions)
of the overall fluorescence intensity minus the background intensity
and the standard errors of the mean as functions of time. After 30
min the fluorescence increased several-fold at pH 9 relative to pH
6 and 7.5. The images were acquired using an objective with 20×
magnification. In this case, the membrane-bound peptide cannot be
separated from the internalized peptide. To measure more strictly
the free intracellular distributed peptide and compare it with these
results, we simultaneously imaged the cells in the dotted regions
using an objective with 60× magnification (Figure S2 in the Supporting Information). We measured the fluorescence
intensity at the nucleolus relative to the background fluorescence
over time and found that the two measurements gave analogous results.
Scale bars = 75 μm.This experiment was performed using an objective with 20×
magnification, allowing the simultaneous visualization of several
cells in the field of view. At this magnification it was difficult
to resolve clearly whether the increase in fluorescence was correlated
with cellular uptake and/or membrane-bound peptides. Therefore, to
be able to differentiate intracellular from membrane-bound peptides
within the same field of view, we switched to a 60× objective
(Figure S2 in the Supporting Information) to capture higher-magnification images of the dotted regions indicated
in Figure 5. The plot in Figure S2 shows the fluorescence intensity in the nucleus
minus the extracellular background fluorescence intensity. It can
be seen that the internalized TATpeptide in the nucleus accumulated
mainly at the nucleolus, from which it becomes easy to recognize that
this fluorescence signal was produced only by free peptides and not
by peptides trapped in endosomes or bound to the cell plasma membrane.
Movies S4–S9 in the Supporting Information show the uptake of 2 μM TATpeptide by HeLa cells at pH 6,
7.5, and 9 taken at 20× and 60× magnification. Cells were
deprived of glucose and nutrients during peptide uptake, and no peptide
trapped in endosomes was detected during this time. Cells tolerated
these conditions, remaining viable. They preserved their morphology
(as shown by differential interference contrast (DIC) images), remained
enzymatically active (Figure S3 in the Supporting
Information), and kept undergoing normal cell division (movie
S10 in the Supporting Information).We also tested the effect of the extracellular pH on the uptake
of multiple RRPs with different lengths, structures, and chirality[8,41−43] using cell lines from different species and kingdoms
(Figures S4–S9 in the Supporting Information). Increasing the extracellular pH resulted in an increase in cellular
peptide uptake for all RRPs by all cell lines. Consistently in all
of the cell lines studied here, at pH 6 there was almost no uptake
of the peptide compared with pH 7.5 and 9. The fact that this behavior
is common to cells from widely separated evolutionary organisms highlights
the universality of the underlying mechanism that drives the cellular
uptake of RRPs.We asked next whether enriching the cells with
fatty acids would
also increase the uptake of RRPs.
Fatty
Acid Plasma Membrane Enrichment Enhances
Uptake of RRPs
Incubating cells in a medium enriched with
fatty acids can increase the cell content of fatty acids.[44,45] Therefore, we first incubated the cells in a medium rich in fatty
acids for 5 min and then washed and incubated the cells in a buffer
at pH 7.5 with different concentrations of the TATpeptide (10, 5,
and 2.5 μM). The cells were then washed and medium plus calcein
was added to monitor for enzymatic activity, and the cells were imaged.
In Figure 6 it can be seen that fatty-acid-enriched
cells display a much higher uptake efficiency than the control cells
and that most of the cells are viable as indicated by their morphology
and enzymatic activity.
Figure 6
Enriching the plasma membrane with fatty acids
enhances the binding
and uptake of arginine-rich peptides. To test whether the cellular
plasma membrane content of fatty acids can alter the uptake efficiency
of RRPs, cells were incubated in a buffer rich in fatty acids for
15 min, washed, and incubated with added RRPs (10, 5, or 2.5 μM)
for 5 min keeping the pH at 7.5. The cells were then washed and regular
cell culture medium plus calcein was added, and the cells were imaged.
In the first column are shown DIC images, in the second column the
fluorescence emission of TAMRA-labeled TAT, in the third column the
fluorescence intensity of calcein, and in the last column the overlay
of the three channels. Scale bar = 25 μm.
Enriching the plasma membrane with fatty acids
enhances the binding
and uptake of arginine-rich peptides. To test whether the cellular
plasma membrane content of fatty acids can alter the uptake efficiency
of RRPs, cells were incubated in a buffer rich in fatty acids for
15 min, washed, and incubated with added RRPs (10, 5, or 2.5 μM)
for 5 min keeping the pH at 7.5. The cells were then washed and regular
cell culture medium plus calcein was added, and the cells were imaged.
In the first column are shown DIC images, in the second column the
fluorescence emission of TAMRA-labeled TAT, in the third column the
fluorescence intensity of calcein, and in the last column the overlay
of the three channels. Scale bar = 25 μm.Polyarginine peptides (>7 amino acids long) efficiently
transduce
into living cells. However, this is not the case for polylysine peptides.[41,46] This is an intriguing result since both arginine and lysine residues
remain positively charged over a broad physiological pH range. Therefore,
fatty acids could analogously mediate the transport of polylysine
peptides. We next asked whether fatty acids would consistently capture
these remarkable differences.
Fatty
Acids Capture Differences between Polyarginine
and Polylysine
If fatty acids indeed play an active role
in the cellular uptake of RRPs, then they should also consistently
show a clear selectivity for arginine over lysine amino acids, making
this a sensible test for the mechanism proposed here. Therefore, we
first looked at the structure and energetics of the interaction between
arginine amino acids (or guanidinium groups) and lysine amino acids
(or amino groups) with the deprotonated carboxyl group of oleic acid.
Using molecular dynamics simulations (Figure 7a), we computed the free energy as a function of the distance between
the carboxyl carbon of oleic acid and the carbon (nitrogen) atom of
the guanidinium (amino) group. This calculation shows that as the
guanidinium group approaches the carboxyl group it encounters a free
energy barrier of 1.8 kJ/mol, and the energy gained upon binding is
8.5 kJ/mol. In contrast, the amino group encounters a much higher
free energy barrier of 6.1 kJ/mol, and the binding energy gain is
only 2.5 kJ/mol. Therefore, guanidinium groups encounter an energetic
barrier more than 3 times weaker to bind fatty acids relative to amino
groups, and the relative gain in energy is more than 3 times higher.
Therefore, guanidinium groups bind more easily to fatty acids and
in doing so gain significantly more energy. Figure 7b shows snapshots of the conformations of an arginine and
a lysine amino acid at the position of the minimum free energy in
each case.
Figure 7
Arginine amino acids have a higher affinity for fatty acids than
lysine amino acids. (a) Computed free energy profiles as functions
of the distance between the carbon atom of the deprotonated carboxyl
acid group (of the oleic acid) and the carbon atom of the guanidium
group (arginine amino acid) or the carbon atom of the amino group
(lysine amino acid). There is a gain in free energy 4 times higher
for the binding of an arginine amino acid to an oleic acid relative
to the binding of a lysine amino acid. (b) Snapshots of conformations
of the amino acids at the positions where the free energy reaches
a minimum, showing a more favorable alignment and hydrogen bonding
in the case of the guanidinium group relative to the amino group.
(c) Hydrophobic absorption of arginine and lysine amino acids at different
pHs and numbers of residues. The photographs show polyarginine and
polylysine peptides labeled with FITC in microcentrifuge tubes composed
of two phases as described in Figure 1. The
absorption into the hydrophobic phase is stronger for polyarginine
peptides than for polylysine peptides. There is a sharp transition
from the aqueous phase to the octanol phase at pH 6.75 for R12, while
in the case of K12 this transition is shifted to a higher pH. Comparing
R12 with R5, the absorption into the hydrophobic phase is shifted
to a higher pH for R5, while K5 is not absorbed into the hydrophobic
phase within this pH range.
Arginine amino acids have a higher affinity for fatty acids than
lysine amino acids. (a) Computed free energy profiles as functions
of the distance between the carbon atom of the deprotonated carboxyl
acid group (of the oleic acid) and the carbon atom of the guanidium
group (arginine amino acid) or the carbon atom of the amino group
(lysine amino acid). There is a gain in free energy 4 times higher
for the binding of an arginine amino acid to an oleic acid relative
to the binding of a lysine amino acid. (b) Snapshots of conformations
of the amino acids at the positions where the free energy reaches
a minimum, showing a more favorable alignment and hydrogen bonding
in the case of the guanidinium group relative to the amino group.
(c) Hydrophobic absorption of arginine and lysine amino acids at different
pHs and numbers of residues. The photographs show polyarginine and
polylysine peptides labeled with FITC in microcentrifuge tubes composed
of two phases as described in Figure 1. The
absorption into the hydrophobic phase is stronger for polyarginine
peptides than for polylysine peptides. There is a sharp transition
from the aqueous phase to the octanol phase at pH 6.75 for R12, while
in the case of K12 this transition is shifted to a higher pH. Comparing
R12 with R5, the absorption into the hydrophobic phase is shifted
to a higher pH for R5, while K5 is not absorbed into the hydrophobic
phase within this pH range.Next, we experimentally tested the fatty acid absorption
of polyarginine
and polylysine peptides of different lengths in the octanol phase.
Figure 7c shows experimental images of the
partition of polyarginine and polylysine peptides between octanol
with 1% oleic acid and aqueous phases at different pHs. We can see
that K12 can be partially absorbed into the octanol phase at a higher
pH than R12. R5 also partitions in the octanol phase at higher pH
than R12, while K5 is unable to partition into the octanol phase within
this pH range. Therefore, the interplay between fatty acids and proton
density captures the essence of the puzzling observations reported
in previous works showing that polylysines or short polyarginine sequences
such as R5 are unable to efficiently transduce into living cells.
Conclusion
Theoretical computations, in vitro
and live-cell experiments reveal
a mechanism in which fatty acids mediate the absorption and transport
of RRPs across a hydrophobic barrier from a high- to a low-pH environment.
This mechanism (depicted in Scheme 1) is essentially
possible in cells because the intracellular pH in most cells is actively
kept near neutral and at this pH plasma membrane fatty acids become
protonated, while at a higher pH they become deprotonated. Deprotonatedfatty acids in contact with the extracellular medium kept at higher
pH bind to guanidinium groups with very high affinity, facilitating
the absorption and peptide transport across the hydrophobic core of
the plasma membrane nucleating a channel. In contact with the lower
cytosolic pH, fatty acids become protonated and neutrally charged,
and the RRPs are released from the plasma membrane into the cells
and the channel closes. Protonated fatty acids freely diffuse across
the plasma membrane, when in contact with the extracellular medium
they get deprotonated, becoming negatively charged and trapped in
the extracellular layer of the plasma membrane. Then, this cycle can
then be repeated.
Scheme 1
Proposed Cellular Uptake Mechanism for Arginine-Rich
Cell-Penetrating
Peptides
(a) The peptide located in
the extracellular medium is attracted and (b) binds to deprotonated
fatty acids. (c) The peptide–fatty acid complex nucleates a
water channel. (d) This peptide–fatty acid complex diffuses
across this channel while simultaneously protons from the cytosolic
side compete for the binding of the guanidinium groups to fatty acids.
(e) The high density of protons in the cytosol protonates the fatty
acids, and the peptide gets released into the cytosol. (f) The channel
closes, and neutral fatty acids freely diffuse across the plasma membrane;
when they come into contact with the extracellular medium, they are
deprotonated. The headgroups of the fatty acids become negatively
charged and trapped in the extracellular layer of the plasma membrane,
and the cycle can repeat again. The inset highlights that essentially
fatty acids are able to get inserted into plasma membrane, transporting
arginine-rich peptides (or guanidinium-rich molecules) toward the
cytosol and protons toward the exterior of the cell. In the cytosol,
fatty acids get protonated, inhibiting the binding of fatty acids
to guanidinium groups.
Proposed Cellular Uptake Mechanism for Arginine-Rich
Cell-Penetrating
Peptides
(a) The peptide located in
the extracellular medium is attracted and (b) binds to deprotonatedfatty acids. (c) The peptide–fatty acid complex nucleates a
water channel. (d) This peptide–fatty acid complex diffuses
across this channel while simultaneously protons from the cytosolic
side compete for the binding of the guanidinium groups to fatty acids.
(e) The high density of protons in the cytosol protonates the fatty
acids, and the peptide gets released into the cytosol. (f) The channel
closes, and neutral fatty acids freely diffuse across the plasma membrane;
when they come into contact with the extracellular medium, they are
deprotonated. The headgroups of the fatty acids become negatively
charged and trapped in the extracellular layer of the plasma membrane,
and the cycle can repeat again. The inset highlights that essentially
fatty acids are able to get inserted into plasma membrane, transporting
arginine-rich peptides (or guanidinium-rich molecules) toward the
cytosol and protons toward the exterior of the cell. In the cytosol,
fatty acids get protonated, inhibiting the binding of fatty acids
to guanidinium groups.The possibility that
these peptides might be able to directly cross
the cell plasma has led, since their discovery, to a search for compounds
that could enhance their cellular uptake. The mechanism outlined here
explains at a fundamental level the enhancement effect of pyrenebutyrate
on the cellular uptake of RRPs. The essential ingredients in the mechanism
presented here are the guanidinium groups, the carboxyl groups coupled
to a hydrophobic moiety, and the pH gradient across the plasma membrane.
Accordingly, increasing any of these ingredients leads to a significant
increase in transduction efficiency.The mechanism uncovered
by these experiments provides a unifying
perspective on the cellular transduction of arginine-rich cell-penetrating
peptides. The simplicity and universality of the elements involved
in this mechanism elegantly reveals how these peptides are able to
efficiently cross in an energy- and receptor-independent manner into
virtually any cell type.
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